<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2016.71002</article-id><article-id pub-id-type="publisher-id">AM-62746</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Design and Analysis of Some Third Order Explicit Almost Runge-Kutta Methods
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>bdulrahman</surname><given-names>Ndanusa</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Khadeejah</surname><given-names>James Audu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Federal University of Technology, Minna, Nigeria</addr-line></aff><pub-date pub-type="epub"><day>11</day><month>01</month><year>2016</year></pub-date><volume>07</volume><issue>01</issue><fpage>13</fpage><lpage>21</lpage><history><date date-type="received"><day>19</day>	<month>December</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>11</month>	<year>January</year>	</date><date date-type="accepted"><day>14</day>	<month>January</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, we propose two new explicit Almost Runge-Kutta (ARK) methods, ARK3 (a three stage third order method, 
  <em>i.e.</em>, 
  <em>s</em> = 
  <em>p</em> = 3) and ARK34 (a four-stage third-order method, 
  <em>i.e.</em>, 
  <em>s</em> = 4, 
  <em>p</em> = 3), for the numerical solution of initial value problems (IVPs). The methods are derived through the application of order and stability conditions normally associated with Runge-Kutta methods; the derived methods are further tested for consistency and stability, a necessary requirement for convergence of any numerical scheme; they are shown to satisfy the criteria for both consistency and stability; hence their convergence is guaranteed. Numerical experiments carried out further justified the efficiency of the methods.
 
</p></abstract><kwd-group><kwd>Almost Runge-Kutta</kwd><kwd> Stability</kwd><kwd> Consistency</kwd><kwd> Convergence</kwd><kwd> Order Conditions</kwd><kwd> Rooted Trees</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>According to [<xref ref-type="bibr" rid="scirp.62746-ref1">1</xref>] the s-stage Runge-Kutta method for solving the initial value problem</p><disp-formula id="scirp.62746-formula272"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x6.png"  xlink:type="simple"/></disp-formula><p>is defined by</p><disp-formula id="scirp.62746-formula273"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x7.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.62746-formula274"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x8.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.62746-formula275"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x9.png"  xlink:type="simple"/></disp-formula><p>Alternative forms of the above equations are:</p><disp-formula id="scirp.62746-formula276"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x10.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.62746-formula277"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x11.png"  xlink:type="simple"/></disp-formula><p>The two forms of Equations (2) and (5) are equivalent by making the interpretation</p><disp-formula id="scirp.62746-formula278"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x12.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x13.png" xlink:type="simple"/></inline-formula> is the inner stages that tend to estimate the solutions at some points; s is the number of stages and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x14.png" xlink:type="simple"/></inline-formula> is the points where the function f is computed for a step. ARK methods are a special class of RK methods that arose out of the quest to develop efficient and accurate methods that have advantages over the traditional methods by retaining the simple stability function of RK methods, allowing minimal information to be passed between steps and adjusting stepsize easily. Since the introduction of ARK methods in by [<xref ref-type="bibr" rid="scirp.62746-ref2">2</xref>] , other researchers who have made their input toward the development of this method include [<xref ref-type="bibr" rid="scirp.62746-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.62746-ref7">7</xref>] .</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Method ARK3 (s = p = 3)</title><p>The general third order three stages Almost Runge-Kutta scheme is of the form:</p><disp-formula id="scirp.62746-formula279"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x15.png"  xlink:type="simple"/></disp-formula><p>We represent the abscissa vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x16.png" xlink:type="simple"/></inline-formula>.</p><p>The order conditions for order three ARK schemes are derived through the standard rooted tree approach used for Runge-Kutta methods [<xref ref-type="bibr" rid="scirp.62746-ref8">8</xref>] .</p><disp-formula id="scirp.62746-formula280"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x17.png"  xlink:type="simple"/></disp-formula><p>The conditions of Runge-Kutta stability for 3<sup>rd</sup> order, 3 stages are:</p><disp-formula id="scirp.62746-formula281"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x18.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula282"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x19.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula283"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x20.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x21.png" xlink:type="simple"/></inline-formula>.</p><p>Acquiring order 2 estimation with respect to 2<sup>nd</sup> scaled derivative for the 3<sup>rd</sup> outgoing solution, we need:</p><disp-formula id="scirp.62746-formula284"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x22.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula285"><label>(14a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x23.png"  xlink:type="simple"/></disp-formula><p>From Equation (12) we have,</p><disp-formula id="scirp.62746-formula286"><label>(14b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x24.png"  xlink:type="simple"/></disp-formula><p>Solving Equation (9) we obtain</p><disp-formula id="scirp.62746-formula287"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x25.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula288"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x26.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula289"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x27.png"  xlink:type="simple"/></disp-formula><p>And from Equation (11), we obtain</p><disp-formula id="scirp.62746-formula290"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x28.png"  xlink:type="simple"/></disp-formula><p>Evaluating both sides of Equation (10) we obtain</p><disp-formula id="scirp.62746-formula291"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x29.png"  xlink:type="simple"/></disp-formula><p>This implies that</p><disp-formula id="scirp.62746-formula292"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x30.png"  xlink:type="simple"/></disp-formula><p>Thus Equation (13) becomes</p><disp-formula id="scirp.62746-formula293"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x31.png"  xlink:type="simple"/></disp-formula><p>Two free parameters, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x32.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x33.png" xlink:type="simple"/></inline-formula> are required for an order three scheme. Thus<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x34.png" xlink:type="simple"/></inline-formula>; and after</p><p>calculating the members of the U matrix we obtain the a scheme for method<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x35.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.62746-formula294"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x36.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2"><title>2.2. Method ARK34 (s = 4, p = 3)</title><p>The third order four stages scheme has the general form:</p><disp-formula id="scirp.62746-formula295"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x37.png"  xlink:type="simple"/></disp-formula><p>Its stability function is expressed as</p><disp-formula id="scirp.62746-formula296"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x38.png"  xlink:type="simple"/></disp-formula><p>The order conditions are derived using the standard rooted tree approach used for Runge-Kutta methods [<xref ref-type="bibr" rid="scirp.62746-ref8">8</xref>] .</p><disp-formula id="scirp.62746-formula297"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x39.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula298"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x40.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula299"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula300"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x42.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula301"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x43.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula302"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x44.png"  xlink:type="simple"/></disp-formula><p>The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x45.png" xlink:type="simple"/></inline-formula> values are obtained by expanding</p><disp-formula id="scirp.62746-formula303"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x46.png"  xlink:type="simple"/></disp-formula><p>Also,</p><disp-formula id="scirp.62746-formula304"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x47.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula305"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x48.png"  xlink:type="simple"/></disp-formula><p>There is also the additional condition</p><disp-formula id="scirp.62746-formula306"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x49.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x50.png" xlink:type="simple"/></inline-formula>and L will be assumed to be the free parameters, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x51.png" xlink:type="simple"/></inline-formula> is the error coefficient comparable to the bushy tree. From Equations (25)-(27) together with Equation (34) we have</p><disp-formula id="scirp.62746-formula307"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x52.png"  xlink:type="simple"/></disp-formula><p>Thus</p><disp-formula id="scirp.62746-formula308"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x53.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula309"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x54.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula310"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x55.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula311"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x56.png"  xlink:type="simple"/></disp-formula><p>From Equation (30) we obtain</p><disp-formula id="scirp.62746-formula312"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x57.png"  xlink:type="simple"/></disp-formula><p>Evaluating the stability matrix of a four stage third order method, we arrive at</p><disp-formula id="scirp.62746-formula313"><label>(41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x58.png"  xlink:type="simple"/></disp-formula><p>where Tr is the trace of a matrix and</p><disp-formula id="scirp.62746-formula314"><label>(42)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x59.png"  xlink:type="simple"/></disp-formula><p>Hence,</p><disp-formula id="scirp.62746-formula315"><label>(43)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x60.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula316"><label>(44)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x61.png"  xlink:type="simple"/></disp-formula><p>And it follows that:</p><disp-formula id="scirp.62746-formula317"><label>(45)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x62.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x63.png" xlink:type="simple"/></inline-formula> we obtain</p><disp-formula id="scirp.62746-formula318"><label>(46)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x64.png"  xlink:type="simple"/></disp-formula><p>We introduce<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x65.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x66.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x67.png" xlink:type="simple"/></inline-formula>. Thus from Equation (46) we arrived at</p><disp-formula id="scirp.62746-formula319"><label>(47)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x68.png"  xlink:type="simple"/></disp-formula><p>And from Equations (32) and (33) we obtain respectively</p><disp-formula id="scirp.62746-formula320"><label>(48)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x69.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula321"><label>(49)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x70.png"  xlink:type="simple"/></disp-formula><p>Further simplification produces the following results</p><disp-formula id="scirp.62746-formula322"><label>(50)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x71.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula323"><label>(51)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x72.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula324"><label>(52)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x73.png"  xlink:type="simple"/></disp-formula><p>Setting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x74.png" xlink:type="simple"/></inline-formula> and substituted this into Equation (29), we obtain</p><disp-formula id="scirp.62746-formula325"><label>(53)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x75.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula326"><label>(54)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula327"><label>(55)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula328"><label>(56)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x78.png"  xlink:type="simple"/></disp-formula><p>Thus</p><disp-formula id="scirp.62746-formula329"><label>(57)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x79.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula330"><label>(58)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x80.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula331"><label>(59)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x81.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula332"><label>(60)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x82.png"  xlink:type="simple"/></disp-formula><p>And the proposed ARK34 with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x83.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.62746-formula333"><label>(61)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x84.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s3"><title>3. Convergence Analysis</title><p>For the method ARK3 represented by Equation (24), the matrix</p><disp-formula id="scirp.62746-formula334"><label>(62)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x85.png"  xlink:type="simple"/></disp-formula><p>must have bounded powers for the method to be stable.</p><p>The characteristic polynomial of V is given as</p><disp-formula id="scirp.62746-formula335"><label>(63)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x86.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula336"><label>(64)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x87.png"  xlink:type="simple"/></disp-formula><p>Thus <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x88.png" xlink:type="simple"/></inline-formula></p><p>Applying Cayley-Hamilton theorem to matrix V</p><disp-formula id="scirp.62746-formula337"><label>(65)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x89.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula338"><label>(66)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x90.png"  xlink:type="simple"/></disp-formula><p>This implies that</p><disp-formula id="scirp.62746-formula339"><label>(67)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x91.png"  xlink:type="simple"/></disp-formula><p>Similarly,</p><disp-formula id="scirp.62746-formula340"><label>(68)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x92.png"  xlink:type="simple"/></disp-formula><p>for every n greater than 2. It implies <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x93.png" xlink:type="simple"/></inline-formula> is bounded, which shows that the method is stable. It is known that methods of order at least one are always consistent; hence the method is consistent since the order of the method is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x94.png" xlink:type="simple"/></inline-formula>. Therefore, Hence the proposed scheme ARK3 is convergent due to the fact that it is both stable and consistent.</p><p>Similarly, for the ARK34 method of Equation (61), the matrix</p><disp-formula id="scirp.62746-formula341"><label>(69)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x95.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.62746-formula342"><label>(70)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x96.png"  xlink:type="simple"/></disp-formula><p>And the eigenvalues are evaluated to be<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x97.png" xlink:type="simple"/></inline-formula>.</p><p>Thus,</p><disp-formula id="scirp.62746-formula343"><label>(71)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x98.png"  xlink:type="simple"/></disp-formula><p>And similarly, it implies that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x99.png" xlink:type="simple"/></inline-formula>, for every n greater than 2. It indicates that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x100.png" xlink:type="simple"/></inline-formula> is bounded which shows that the method is stable. Also, the method is consistent since it is of order 3, i.e.,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x101.png" xlink:type="simple"/></inline-formula>. Hence the proposed scheme (ARK34) is convergent due to the fact that it is both stable and consistent.</p></sec><sec id="s4"><title>4. Numerical Examples</title><p>Considering the problem below:</p><disp-formula id="scirp.62746-formula344"><label>(72)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403017x102.png"  xlink:type="simple"/></disp-formula><p>Source: Rattenbury [<xref ref-type="bibr" rid="scirp.62746-ref3">3</xref>] .</p><p>Problem (72) is solved using the proposed ARK34 method. The results are obtained and compared with similar ARK34 methods of [<xref ref-type="bibr" rid="scirp.62746-ref3">3</xref>] and [<xref ref-type="bibr" rid="scirp.62746-ref5">5</xref>] respectively and presented in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Comparison of ARK34 with other methods (h = 0.1)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-7403017x103.png"/></fig><p>From <xref ref-type="fig" rid="fig1">Figure 1</xref> it is evident that our Proposed ARK34 method performed better than the methods of [<xref ref-type="bibr" rid="scirp.62746-ref3">3</xref>] and [<xref ref-type="bibr" rid="scirp.62746-ref5">5</xref>] since it exhibits lesser error than the errors of the existing methods.</p></sec><sec id="s5"><title>5. Conclusion</title><p>Two ARK methods are proposed, ARK3 <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x104.png" xlink:type="simple"/></inline-formula> and ARK34<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403017x105.png" xlink:type="simple"/></inline-formula>. The methods have been proven to be consistent and stable, thereby guaranteeing their convergence. This is further illustrated by comparing the performance of one of the methods with other methods of similar order. The proposed method ARK34 is shown to perform better than the existing methods.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors would like to thank the reviewer(s) for their constructive criticisms.</p></sec><sec id="s7"><title>Cite this paper</title><p>AbdulrahmanNdanusa,Khadeejah JamesAudu, (2016) Design and Analysis of Some Third Order Explicit Almost Runge-Kutta Methods. Applied Mathematics,07,13-21. doi: 10.4236/am.2016.71002</p></sec></body><back><ref-list><title>References</title><ref id="scirp.62746-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Lambert, J.D. (1991) Numerical Method for Ordinary Differential Systems: The Initial Value Problem. John Wiley &amp; Sons Ltd., New York.</mixed-citation></ref><ref id="scirp.62746-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Butcher, J.C. (1997) An Introduction to Almost Runge-Kutta Methods. Applied Numerical Mathematics, 24, 331-342. 
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